Due to plasma damping, the validity of the perturbative expansion of the effective potential breaks down
at high temperatures. A remedy to this problem is to resum the daisy diagrams to all orders,
which results in an additional contribution to the bosonic masses [1]}.
Thus, we replace the field-dependent bosonic masses at finite temperatures by
\(M_i^2(h,s)\rightarrow M_i^2(h,s,T)=M_i^2(h,s)+\Pi _i(T),\) 
